Geiger-Marsden Experiment (Rutherford Scattering)
- The experiment measured the number of alpha particles (\( N \)) scattered at different angles (\( \theta \)).
- The observed scattering pattern led to significant conclusions about atomic structure.
Graph: Variation of \( N \) with \( \theta \)
Conclusions from the Graph
1. Most alpha particles pass undeflected, meaning the atom is mostly empty space.
2. Few particles are scattered at large angles, implying a small, dense, positively charged nucleus. Expression for Distance of Closest Approach The distance of closest approach (\( r_0 \)) is the minimum separation between the alpha particle and the nucleus before it stops and reverses.
- At the point of closest approach, the initial kinetic energy of the alpha particle is converted into electrostatic potential energy: \[ \frac{1}{2} m v^2 = \frac{1}{4\pi\epsilon_0} \frac{Z e \cdot 2e}{r_0} \]
Solving for \( r_0 \): \[ r_0 = \frac{1}{4\pi\epsilon_0} \frac{2 Z e^2}{\frac{1}{2} m v^2} \] \[ r_0 = \frac{4 \pi \epsilon_0 \cdot 2 Z e^2}{m v^2} \] Thus, the distance of closest approach is: \[ r_0 = \frac{2 Z e^2}{4 \pi \epsilon_0 \cdot \frac{1}{2} m v^2} \]
This represents the minimum distance between the alpha particle and the nucleus before repulsion stops its motion.